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String Theory and M-Theory

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9.8 Nonperturbative effects in Calabi–Yau compactifications 403<br />

Let us use the same SU(3) covariant notation as in the previous exercise.<br />

Compactification on a Calabi–Yau three-fold again gives N = 2, D = 4<br />

supersymmetry. The fields belong to the following supermultiplets:<br />

gravity multiplet : Gµν, Ψµ, Ψµ, Cµijk<br />

h 2,1 vector supermultiplets : C µij ¯ k , Gij, fermions<br />

h 1,1 hypermultiplets : C µνi¯j, G i¯j, B i¯j, C i¯j, fermions<br />

universal hypermultiplet : Φ, C, Bµν, Cµν, fermions.<br />

Now taking into account that Gij is complex <strong>and</strong> that the four-form C has a<br />

self-duality constraint on its field strength, the total number of the massless<br />

scalar fields is 2h 2,1 + 4(h 1,1 + 1). The total number of massless vector fields<br />

is h 2,1 + 1. ✷<br />

9.8 Nonperturbative effects in Calabi–Yau compactifications<br />

Until now we have discussed perturbative aspects of Calabi–Yau compactification<br />

that were understood prior to the second superstring revolution.<br />

This section <strong>and</strong> the following ones discuss some nonperturbative aspects<br />

of Calabi–Yau compactifications that were discovered during <strong>and</strong> after the<br />

second superstring revolution.<br />

The conifold singularity<br />

In addition to their nonuniqueness, one of the main problems with Calabi–<br />

Yau compactifications is that their moduli spaces contain singularities, that<br />

is, points in which the classical description breaks down. By analyzing a<br />

particular example of such a singularity, the conifold singularity, it became<br />

clear that the classical low-energy effective action description breaks down.<br />

Nonperturbative effects due to branes wrapping vanishing (or degenerating)<br />

cycles have to be taken into account.<br />

To be concrete, let us consider the type IIB theory compactified on a<br />

Calabi–Yau three-fold. As we have seen in the previous section, the moduli<br />

space M2,1 (M) can be described in terms of homogeneous special coordinates<br />

XI . A conifold singularity appears when one of the coordinates, say<br />

X 1 <br />

= Ω, (9.140)<br />

vanishes. The period of Ω over A 1 goes to zero, <strong>and</strong> therefore A 1 is called<br />

A 1

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